Question
If an $AC$ main supply is given to be $220\,V$. The average $emf$ during a positive half cycle will be.....$V$
$\therefore \mathrm{E}_{\mathrm{rms}}=\frac{\mathrm{E}_{0}}{\sqrt{2}} \Rightarrow \mathrm{E}_{0}=\sqrt{2} \mathrm{E}_{\mathrm{rms}}$
Average e.m.f over half cycle
$=\frac{2}{\pi} \mathrm{E}_{0}=0.637 \times 1.41 \times 220=198.15 \mathrm{\,V}$
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X-rays b. y-rays c. UV waves d. Microwaves.
| List-I | List-II |
| (A) Biot-Savart's law | (i) $\frac{\mu_0 I_1 I_2}{2 \pi d}$ |
| B) Ampere's circuit law | (ii) $q [\vec{ E }+(\vec{ V } \times \vec{ B })]$ |
| C) Force between two parallel current carrying conductors | (iii) $\oint \overline{ B } \cdot \overline{ dl }=\mu_0 \Sigma i$ |
| (D) Lorentz force | (iv) $\vec{B}=\frac{\mu_0 i}{4 \pi} \int \frac{d l \sin \theta}{r^2} \hat{n}$ |

$\left[\right.$ Given $\left.g=10 \,ms ^{-2}\right]$